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361 |
\section{Non-linear advection schemes} |
\section{Non-linear advection schemes} |
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|
\label{sect:non-linear_advection_schemes} |
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\begin{rawhtml} |
\begin{rawhtml} |
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\tau^{n+1/3} & = & \tau^{n} |
\tau^{n+1/3} & = & \tau^{n} |
629 |
- \Delta t \left( \frac{1}{\Delta x} \delta_i F^x(\tau^{n}) |
- \Delta t \left( \frac{1}{\Delta x} \delta_i F^x(\tau^{n}) |
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+ \tau^{n} \frac{1}{\Delta x} \delta_i u \right) \\ |
+ \tau^{n} \frac{1}{\Delta x} \delta_i u \right) \\ |
631 |
\tau^{n+2/3} & = & \tau^{n} |
\tau^{n+2/3} & = & \tau^{n+1/3} |
632 |
- \Delta t \left( \frac{1}{\Delta y} \delta_j F^y(\tau^{n+1/3}) |
- \Delta t \left( \frac{1}{\Delta y} \delta_j F^y(\tau^{n+1/3}) |
633 |
+ \tau^{n} \frac{1}{\Delta y} \delta_i v \right) \\ |
+ \tau^{n} \frac{1}{\Delta y} \delta_i v \right) \\ |
634 |
\tau^{n+3/3} & = & \tau^{n} |
\tau^{n+3/3} & = & \tau^{n+2/3} |
635 |
- \Delta t \left( \frac{1}{\Delta r} \delta_k F^x(\tau^{n+2/3}) |
- \Delta t \left( \frac{1}{\Delta r} \delta_k F^x(\tau^{n+2/3}) |
636 |
+ \tau^{n} \frac{1}{\Delta r} \delta_i w \right) |
+ \tau^{n} \frac{1}{\Delta r} \delta_i w \right) |
637 |
\end{eqnarray} |
\end{eqnarray} |
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|
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\end{minipage} } |
\end{minipage} } |
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\begin{figure} |
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\resizebox{3.5in}{!}{\includegraphics{part2/multiDim_CS.eps}} |
670 |
|
\caption{Muti-dimensional advection time-stepping with Cubed-Sphere topology |
671 |
|
\label{fig:advect-multidim_cs} |
672 |
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} |
673 |
|
\end{figure} |
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|
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\section{Comparison of advection schemes} |
\section{Comparison of advection schemes} |
676 |
|
\label{sect:tracer_advection_schemes} |
677 |
\begin{rawhtml} |
\begin{rawhtml} |
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Advection Scheme & code & use & use Multi- & Stencil & comments \\ |
Advection Scheme & code & use & use Multi- & Stencil & comments \\ |
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& & A.B. & dimension & (1 dim) & \\ |
& & A.B. & dimension & (1 dim) & \\ |
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\hline \hline |
\hline \hline |
688 |
|
$1^{rst}$order upwind & 1 & No & Yes & 3 pts & linear/$\tau$, non-linear/v\\ |
689 |
|
\hline |
690 |
centered $2^{nd}$order & 2 & Yes & No & 3 pts & linear \\ |
centered $2^{nd}$order & 2 & Yes & No & 3 pts & linear \\ |
691 |
\hline |
\hline |
692 |
$3^{rd}$order upwind & 3 & Yes & No & 5 pts & linear/tracer\\ |
$3^{rd}$order upwind & 3 & Yes & No & 5 pts & linear/$\tau$\\ |
693 |
\hline |
\hline |
694 |
centered $4^{th}$order & 4 & Yes & No & 5 pts & linear \\ |
centered $4^{th}$order & 4 & Yes & No & 5 pts & linear \\ |
695 |
\hline \hline |
\hline \hline |
696 |
% Lax-Wendroff & 10 & No & Yes & 3 pts & linear/tracer, non-linear/flow\\ |
$2^{nd}$order DST (Lax-Wendroff) & 20 & |
697 |
% \hline |
No & Yes & 3 pts & linear/$\tau$, non-linear/v\\ |
698 |
$3^{rd}$order DST & 30 & No & Yes & 5 pts & linear/tracer, non-linear/flow\\ |
\hline |
699 |
|
$3^{rd}$order DST & 30 & No & Yes & 5 pts & linear/$\tau$, non-linear/v\\ |
700 |
\hline \hline |
\hline \hline |
701 |
$2^{nd}$order Flux Limiters & 77 & No & Yes & 5 pts & non-linear \\ |
$2^{nd}$order Flux Limiters & 77 & No & Yes & 5 pts & non-linear \\ |
702 |
\hline |
\hline |
706 |
\caption{Summary of the different advection schemes available in MITgcm. |
\caption{Summary of the different advection schemes available in MITgcm. |
707 |
``A.B.'' stands for Adams-Bashforth and ``DST'' for direct space time. |
``A.B.'' stands for Adams-Bashforth and ``DST'' for direct space time. |
708 |
The code corresponds to the number used to select the corresponding |
The code corresponds to the number used to select the corresponding |
709 |
advection scheme in the parameter file (e.g., {\em tempAdvScheme=3} in |
advection scheme in the parameter file (e.g., {\bf tempAdvScheme}=3 in |
710 |
file {\em data} selects the $3^{rd}$ order upwind advection scheme |
file {\em data} selects the $3^{rd}$ order upwind advection scheme |
711 |
for temperature). |
for temperature). |
712 |
} |
} |